|Publication number||US7514367 B2|
|Application number||US 11/382,739|
|Publication date||Apr 7, 2009|
|Filing date||May 11, 2006|
|Priority date||Jun 17, 2005|
|Also published as||US20060286743|
|Publication number||11382739, 382739, US 7514367 B2, US 7514367B2, US-B2-7514367, US7514367 B2, US7514367B2|
|Inventors||Hsiang Lan Lung, ChiaHua Ho, Shih Hung Chen, Chieh Fang Chen|
|Original Assignee||Macronix International Co., Ltd.|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (101), Non-Patent Citations (35), Referenced by (1), Classifications (24), Legal Events (3)|
|External Links: USPTO, USPTO Assignment, Espacenet|
The present application is a continuation-in-part of U.S. patent application Ser. No. 11/155,067; filed 17 Jun. 2005, which is incorporated by reference as if fully set forth herein.
International Business Machines Corporation, a New York corporation; Macronix International Corporation, Ltd., a Taiwan corporation, and Infineon Technologies A.G., a German corporation, are parties to a Joint Research Agreement.
1. Field of the Invention
The present invention relates to manufacturing methods for integrated circuits, including methods for making a narrow structure on a substrate, such as a narrow line of phase change material.
2. Description of Related Art
Phase change based memory materials are widely used in read-write optical disks. These materials have at least two solid phases, including for example a generally amorphous solid phase and a generally crystalline solid phase. Laser pulses are used in read-write optical disks to switch between phases and to read the optical properties of the
Phase change based memory materials, like chalcogenide based materials and similar materials, also can be caused to change phase by application of electrical current at levels suitable for implementation in integrated circuits. The generally amorphous state is characterized by higher resistivity than the generally crystalline state, which can be readily sensed to indicate data. These properties have generated interest in using programmable resistive material to form nonvolatile memory circuits, which can be read and written with random access.
The change from the amorphous to the crystalline state is generally a lower current operation. The change from crystalline to amorphous, referred to as reset herein, is generally a higher current operation, which includes a short high current density pulse to melt or breakdown the crystalline structure, after which the phase change material cools quickly, quenching the phase change process, allowing at least a portion of the phase change structure to stabilize in the amorphous state. It is desirable to minimize the magnitude of the reset current used to cause transition of phase change material from crystalline state to amorphous state. The magnitude of the reset current needed for reset can be reduced by reducing the size of the phase change material element in the cell and of the contact area between electrodes and the phase change material, so that higher current densities are achieved with small absolute current values through the phase change material element.
One direction of development has been toward forming small pores in an integrated circuit structure, and using small quantities of programmable resistive material to fill the small pores. Patents illustrating development toward small pores include: Ovshinsky, “Multibit Single Cell Memory Element Having Tapered Contact,” U.S. Pat. No. 5,687,112, issued Nov. 11, 1997; Zahorik et al., “Method of Making Chalogenide [sic] Memory Device,” U.S. Pat. No. 5,789,277, issued Aug. 4, 1998; Doan et al., “Controllable Ovonic Phase-Change Semiconductor Memory Device and Methods of Fabricating the Same,” U.S. Pat. No. 6,150,253, issued Nov. 21, 2000.
It is desirable therefore to provide a memory cell structure having small dimensions and low reset currents, and a method for manufacturing such structure that meets tight process variation specifications needed for large-scale memory devices. It is further desirable to provide a manufacturing process and a structure which are compatible with manufacturing of peripheral circuits on the same integrated circuit. Also, manufacturing techniques for making nano-scale structures on integrated circuits and other substrates are needed.
Technology described herein includes a memory device comprising a first electrode having a top side, a second electrode having a top side and an insulating member between the first electrode and the second electrode. The insulating member has a thickness between the first and second electrodes near the top side of the first electrode and the top side of the second electrode. A thin film bridge crosses the insulating member, and defines an inter-electrode path between the first and second electrodes across the insulating member. The inter-electrode path across the insulating member has a path length defined by the width of the insulating member.
The volume of memory material subject of phase change can be very small, determined by the thickness of the insulating member (path length in the x-direction), the thickness of the thin film used to form the bridge (y-direction), and the width of the bridge orthogonal to the path length (z-direction). The thickness of the insulating member and the thickness of the thin film of memory material used to form the bridge are determined in embodiments of the technology by thin film thicknesses which are not limited by the lithographic processes used in manufacturing the memory cell. The width of the bridge is also smaller than a minimum feature size F that is specified for a lithographic process used in patterning the layer of material in embodiments of the present invention. Techniques for manufacturing the bridge, and defining the width of the bridge of memory material are described, which are based on forming and using a sidewall etch mask structure.
In an embodiment of the manufacturing method, the bridges of memory material are made by a process comprising a number of steps including the following:
The sidewall etch mask can be used in a variety of processes to define the width of the line of material. One example process includes first etching the layer of first material using the first side of the sidewall etch mask and the pattern on the second side of the sidewall etch mask in the layer of pattern material as a combined etch mask; then removing the pattern material from the second side of the sidewall etch mask; and second etching remaining portions of the layer of first material using the second side of the sidewall etch mask to leave the line of the first material.
In another example process, the pattern material is removed from the second side of the sidewall etch mask, and then the layer of first material is etched using the first and second sides of the sidewall etch mask to leave the line of the first material.
In yet another alternative process, the layer of first material is first etched using the first side of the sidewall etch mask and the pattern on the second side of the sidewall etch mask in the layer of pattern material as a combined etch mask. Then a second sidewall material is deposited over the sidewall etch mask, and etched to form a covering sidewall over the sidewall etch mask. The pattern material is then removed from the second side of the sidewall etch mask, and remaining portions of the first material are etched using the second side of the sidewall etch mask to leave the line of the first material. The covering sidewall protects the side of the line of first material first etched using the first side of the sidewall etch mask from damage during the second etch.
The method described herein for formation of the bridge for use in a memory cell can be used to make a very small bridge for other uses. Nano-technology devices with very small bridge structures are provided using materials other than phase change to materials, like metals, dielectrics, organic materials, semiconductors, and so on.
Other aspects and advantages of the invention are shown in the following.
A detailed description of thin film fuse phase change memory cells and methods for manufacturing such memory cells and other narrow structures is provided with reference to
Access circuitry can be implemented to contact the first electrode 12 and the second electrode 13 in a variety of configurations for controlling the operation of the memory cell, so that it can be programmed to set the bridge 11 in one of the two solid phases that can be reversibly implemented using the memory material. For example, using a chalcogenide-based phase change memory material, the memory cell may be set to a relatively high resistivity state in which at least a portion of the bridge in the current path is in an amorphous state, and a relatively low resistivity state in which most of the bridge in the current path is in a crystalline state.
As can be appreciated, the active channel in the bridge of memory material can be made extremely small in the illustrated structure, reducing the magnitude of current needed to induce the phase changes.
Likewise, the bridge thickness T (y-dimension) can be very small in embodiments of the memory cell. This bridge thickness T can be established using a thin film deposition technique on the top surfaces of the first electrode 12, insulating member 14, and second electrode 13. Thus, embodiments of the memory cell have a bridge thickness T about 30 nm or less. Other embodiments of the memory cell have a bridge thickness of about 20 nm or less. In yet other embodiments, the bridge thickness T is about 10 nm or less. It will be understood that the bridge thickness T can be even smaller than 10 nm, using thin film deposition techniques such as atomic layer deposition and the like, according to the needs of the particular application, so long as the thickness is sufficient for the bridge to perform its purpose as memory element having at least two solid phases, reversible by a current or by a voltage applied across the first and second electrodes.
As illustrated in
Embodiments of the memory cell include phase change based memory materials, including chalcogenide based materials and other materials, for the bridge 11. Chalcogens include any of the four elements oxygen (O), sulfur (S), selenium (Se), and tellurium (Te), forming part of group VI of the periodic table. Chalcogenides comprise compounds of a chalcogen with a more electropositive element or radical. Chalcogenide alloys comprise combinations of chalcogenides with other materials such as transition metals. A chalcogenide alloy usually contains one or more elements from column six of the periodic table of elements, such as germanium (Ge) and tin (Sn). Often, chalcogenide alloys include combinations including one or more of antimony (Sb), gallium (Ga), indium (In), and silver (Ag). Many phase change based memory materials have been described in technical literature, including alloys of: Ga/Sb, In/Sb, In/Se, Sb/Te, Ge/Te, Ge/Sb/Te, In/Sb/Te, Ga/Se/Te, Sn/Sb/Te, In/Sb/Ge, Ag/In/Sb/Te, Ge/Sn/Sb/Te, Ge/Sb/Se/Te and Te/Ge/Sb/S. In the family of Ge/Sb/Te alloys, a wide range of alloy compositions may be workable. The compositions can be characterized as TeaGebSb100−(a+b). One researcher has described the most useful alloys as having an average concentration of Te in the deposited materials well below 70%, typically below about 60% and ranged in general from as low as about 23% up to about 58% Te and most preferably about 48% to 58% Te. Concentrations of Ge were above about 5% and ranged from a low of about 8% to about 30% average in the material, remaining generally below 50%. Most preferably, concentrations of Ge ranged from about 8% to about 40%. The remainder of the principal constituent elements in this composition was Sb. These percentages are atomic percentages that total 100% of the atoms of the constituent elements. (Ovshinsky '112 patent, cols 10-11.) Particular alloys evaluated by another researcher include Ge2Sb2Te5, GeSb2Te4 and GeSb4Te7 (Noboru Yamada, “Potential of Ge—Sb—Te Phase-Change Optical Disks for High-Data-Rate Recording”, SPIE v.3109, pp. 28-37 (1997).) More generally, a transition metal such as chromium (Cr), iron (Fe), nickel (Ni), niobium (Nb), palladium (Pd), platinum (Pt) and mixtures or alloys thereof may be combined with Ge/Sb/Te to form a phase change alloy that has programmable resistive properties. Specific examples of memory materials that may be useful are given in Ovshinsky '112 at columns 11-13, which examples are hereby incorporated by reference.
Phase change alloys are capable of being switched between a first structural state in which the material is in a generally amorphous solid phase, and a second structural state in which the material is in a generally crystalline solid phase in its local order in the active channel region of the cell. These alloys are at least bistable. The term amorphous is used to refer to a relatively less ordered structure, more disordered than a single crystal, which has the detectable characteristics such as higher electrical resistivity than the crystalline phase. The term crystalline is used to refer to a relatively more ordered structure, more ordered than in an amorphous structure, which has detectable characteristics such as lower electrical resistivity than the amorphous phase. Typically, phase change materials may be electrically switched between different detectable states of local order across the spectrum between completely amorphous and completely crystalline states. Other material characteristics affected by the change between amorphous and crystalline phases include atomic order, free electron density and activation energy. The material may be switched either into different solid phases or into mixtures of two or more solid phases, providing a gray scale between completely amorphous and completely crystalline states. The electrical properties in the material may vary accordingly.
Phase change alloys can be changed from one phase state to another by application of electrical pulses. It has been observed that a shorter, higher amplitude pulse tends to change the phase change material to a generally amorphous state. A longer, lower amplitude pulse tends to change the phase change material to a generally crystalline state. The energy in a shorter, higher amplitude pulse is high enough to allow for bonds of the crystalline structure to be broken and short enough to prevent the atoms from realigning into a crystalline state. Appropriate profiles for pulses can be determined, without undue experimentation, specifically adapted to a particular phase change alloy. In following sections of the disclosure, the phase change material is referred to as GST, and it will be understood that other types of phase change materials can be used. A material useful for implementation of a memory cell as described herein is Ge2Sb2Te5.
Other programmable resistive memory materials may be used in other embodiments of the invention, including N2 doped GST, GexSby, or other material that uses different crystal phase changes to determine resistance; PrxCayMnO3, PrSrMnO, ZrOx, or other material that uses an electrical pulse to change the resistance state; 7,7,8,8-tetracyanoquinodimethane (TCNQ), methanofullerene 6,6-phenyl C61-butyric acid methyl ester (PCBM), TCNQ-PCBM, Cu-TCNQ, Ag-TCNQ, C60-TCNQ, TCNQ doped with other metal, or any other polymer material that has bistable or multi-stable resistance state controlled by an electrical pulse.
The following are short summaries describing four types of resistive memory materials. The first type is chalcogenide material, such as GexSbyTez where x:y:z=2:2:5, or other compositions with x: 0˜5; y: 0˜5; z: 0˜10. GeSbTe with doping, such as N—, Si—, Ti—, or other element doping is alternatively used.
An exemplary method for forming chalcogenide material uses PVD-sputtering or magnetron-sputtering method with source gas(es) of Ar, N2, and/or He, etc. at the pressure of 1 mTorr ˜100 mTorr. The deposition is usually done at room temperature. A collimater with an aspect ratio of 1˜5 can be used to improve the fill-in performance. To improve the fill-in performance, a DC bias of several tens of volts to several hundreds of volts is also used. On the other hand, the combination of DC bias and the collimater can be used simultaneously.
A post-deposition annealing treatment in vacuum or in an N2 ambient is optionally performed to improve the crystallize state of chalcogenide material. The annealing temperature typically ranges from 100° C. to 400° C. with an anneal time of less than 30 minutes.
The thickness of chalcogenide material depends on the design of cell structure. In general, a chalcogenide material with thickness of higher than 8 nm can have a phase change characterization so that the material exhibits at least two stable resistance states.
A second type of memory material suitable for use in embodiments is colossal magnetoresistance (“CMR”) material, such as Prx,CayMnO3 where x:y=0.5:0.5, or other compositions with x:0˜1; y:0˜1. CMR material that includes Mn oxide is alternatively used.
An exemplary method for forming CMR material uses PVD sputtering or magnetron-sputtering method with source gases of Ar, N2, O2, and/or He, etc. at the pressure of 1 mTorr˜100 mTorr. The deposition temperature can range from room temperature to ˜600° C., depending on the post deposition treatment condition. A collimater with an aspect ratio of 1˜5 can be used to improve the fill-in performance. To improve the fill-in performance, the DC bias of several tens of volts to several hundreds of volts is also used. On the other hand, the combination of DC bias and the collimater can be used simultaneously. A magnetic field of several tens of Gauss to as much as a Tesla (10,000 Gauss) may be applied to improve the magnetic crystallized phase.
A post-deposition annealing treatment in vacuum or in an N2 ambient or O2/N2 mixed ambient is optionally used to improve the crystallized state of CMR material. The annealing temperature typically ranges from 400° C. to 600° C. with an anneal time of less than 2 hours.
The thickness of CMR material depends on the design of the cell structure. The CMR thickness of 10 nm to 200 nm can be used for the core material. A buffer layer of YBCO (YBaCuO3, which is a type of high temperature superconductor material) is often used to improve the crystallized state of CMR material. The YBCO is deposited before the deposition of CMR material. The thickness of YBCO ranges from 30 nm to 200 nm.
A third type of memory material is two-element compounds, such as NixOy; Tix,Oy; AlxOy; WxOy; ZnxOy; ZrxOy; CuxOy; etc, where x:y=0.5:0.5, or other compositions with x:0˜1; y:0˜1. An exemplary formation method uses a PVD sputtering or magnetron-sputtering method with reactive gases of Ar, N2, O2, and/or He, etc. at the pressure of 1 mTorr˜100 mTorr, using a target of metal oxide, such as NixOy; Tix, Oy; AlxOy; WxOy; ZnxOy; ZrxOy; CuxOy; etc. The deposition is usually done at room temperature. A collimater with an aspect ratio of 1˜5 can be used to improve the fill-in performance. To improve the fill-in performance, the DC bias of several tens of volts to several hundreds of volts is also used. If desired, the combination of DC bias and the collimater can be used simultaneously.
A post-deposition annealing treatment in vacuum or in an N2 ambient or O2/N2 mixed ambient is optionally performed to improve the oxygen distribution of metal oxide. The annealing temperature ranges from 400° C. to 600° C. with an anneal time of less than 2 hours.
An alternative formation method uses a PVD sputtering or magnetron-sputtering method with reactive gases of Ar/O2, Ar/N2/O2, pure O2, He/O2, He/N2/O2 etc. at the pressure of 1 mTorr˜100 mTorr, using a target of metal oxide, such as Ni, Ti, Al, W, Zn, Zr, or Cu etc. The deposition is usually done at room temperature. A collimater with an aspect ratio of 1˜5 can be used to improve the fill-in performance. To improve the fill-in performance, a DC bias of several tens of volts to several hundreds of volts is also used. If desired, the combination of DC bias and the collimater can be used simultaneously.
A post-deposition annealing treatment in vacuum or in an N2 ambient or O2/N2 mixed ambient is optionally performed to improve the oxygen distribution of metal oxide. The annealing temperature ranges from 400° C. to 600° C. with an anneal time of less than 2 hours.
Yet another formation method uses oxidation by a high temperature oxidation system ,such as a furnace or a rapid thermal pulse (“RTP”) system. The temperature ranges from 200° C. to 700° C. with pure O2 or N2/O2 mixed gas at a pressure of several mTorr to 1 atm. The time can range several minute to hours. Another oxidation method is plasma oxidation. An RF or a DC source plasma with pure O2 or Ar/O2 mixed gas or Ar/N2/O2 mixed gas at a pressure of 1 mTorr to 100 mTorr is used to oxidize the surface of metal, such as Ni, Ti, Al, W, Zn, Zr, or Cu etc. The oxidation time ranges several seconds to several minutes. The oxidation temperature ranges from room temperature to 300° C., depending on the degree of plasma oxidation.
A fourth type of memory material is a polymer material, such as TCNQ with doping of Cu, C60, Ag etc. or PCBM-TCNQ mixed polymer. One formation method uses evaporation by thermal evaporation, e-beam evaporation, or molecular beam epitaxy (“MBE”) system. A solid-state TCNQ and dopant pellets are co-evaporated in a single chamber. The solid-state TCNQ and dopant pellets are put in a W-boat or a Ta-boat or a ceramic boat. A high electrical current or an electron-beam is applied to melt the source so that the materials are mixed and deposited on wafers. There are no reactive chemistries or gases. The deposition is done at a pressure of 10−4 Torr to 10−10 Torr. The wafer temperature ranges from room temperature to 200° C.
A post-deposition annealing treatment in vacuum or in an N2 ambient is optionally performed to improve the composition distribution of polymer material. The annealing temperature ranges from room temperature to 300° C. with an anneal time of less than 1 hour.
Another technique for forming a layer of polymer-based memory material is to use a spin-coater with doped-TCNQ solution at a rotation of less than 1000 rpm. After spin-coating, the wafer is held (typically at room temperature or temperature less than 200° C.) for a time sufficient for solid-state formation. The hold time ranges from several minutes to days, depending on the temperature and on the formation conditions.
FIGS. 2 through 10A-10B illustrate a technique for making narrow lines of material on a substrate, which can be applied to manufacturing the bridges of memory material over an electrode layer as described herein. As shown in
Next, as shown in
While the present invention is disclosed by reference to the preferred embodiments and examples detailed above, it is to be understood that these examples are intended in an illustrative rather than in a limiting sense. It is contemplated that modifications and combinations will occur to those skilled in the art, which modifications and combinations will be within the spirit of the invention and the scope of the following claims.
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|Citing Patent||Filing date||Publication date||Applicant||Title|
|US9256126||Oct 31, 2013||Feb 9, 2016||Irresistible Materials Ltd||Methanofullerenes|
|U.S. Classification||438/734, 438/84, 438/584, 438/595, 438/3, 438/95, 438/947|
|Cooperative Classification||H01L45/148, H01L45/14, H01L45/144, H01L45/1625, Y10S438/947, H01L45/06, H01L45/04, H01L45/146, H01L45/1226, H01L45/1675, H01L45/1691, G11C13/0004, H01L45/1641, H01L45/147|
|European Classification||H01L45/04, H01L27/24|
|Oct 4, 2006||AS||Assignment|
Owner name: MACRONIX INTERNATIONAL CO., LTD., TAIWAN
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